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Friction of flat and micropatterned interfaces with nanoscale roughness

机译:具有纳米级粗糙度的扁平和微图案界面的摩擦

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摘要

The dry friction of surfaces with nanoscale roughness and the possibility of using micropatterning to tailor friction by manipulating contact area is investigated. Square wave patterns produced on samples from silicon wafers (and their unstructured equivalent) were slid against unstructured silicon counter surfaces. The width of the square wave features was adjusted to vary the apparent feature contact area. The existence of nanoscale roughness was sufficient to ensure Amontons' first law (F = mu P) on both structured & unstructured samples. Somewhat counterintuitively, friction was independent of the apparent feature contact area making it difficult to tailor friction via the feature contact area. This occurred because, even though the apparent feature contact area was adjusted, the surface roughness and nominal flatness at the contact interface was preserved ensuring that the real contact area and thereby the friction, were likewise preserved. This is an interesting special case, but not universally applicable: friction can indeed be adjusted by structuring provided the intervention leads to a change in real contact area (or interlocking)- and this depends on the specific surface geometry and topography.
机译:研究了具有纳米级粗糙度的表面的干摩擦以及利用微图案通过操纵接触面积来调整摩擦的可能性。硅片(及其非结构等效物)样品上产生的方波图案在非结构硅台面上滑动。调整方波特征的宽度,以改变明显的特征接触面积。纳米级粗糙度的存在足以确保阿蒙顿第一定律(F=mu P)适用于结构化和非结构化样品。在某种程度上,与直觉相反,摩擦力与表面特征接触区域无关,因此很难通过特征接触区域调整摩擦力。这是因为,即使调整了表面特征接触面积,接触界面处的表面粗糙度和标称平整度也得到了保留,从而确保了真实接触面积和摩擦力也得到了同样的保留。这是一个有趣的特例,但并非普遍适用:只要干预导致实际接触面积(或连锁)发生变化,摩擦确实可以通过结构进行调整,这取决于具体的表面几何形状和地形。

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